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@ARTICLE{FernndezDelgado:878293,
author = {Fernández-Delgado, N. and Herrera, M. and Delgado, F. J.
and Tavabi, A. H. and Luysberg, M. and Dunin-Borkowski, R.
E. and Juárez-Pérez, E. J. and Hames, B Clasen and
Mora-Sero, I. and Suárez, I. and Martínez-Pastor, J. P.
and Molina, S. I.},
title = {{S}tructural characterization of bulk and nanoparticle lead
halide perovskite thin films by ({S}){TEM} techniques},
journal = {Nanotechnology},
volume = {30},
number = {13},
issn = {1361-6528},
address = {Bristol},
publisher = {IOP Publ.},
reportid = {FZJ-2020-02756},
pages = {135701 -},
year = {2019},
abstract = {Lead halide (APbX3) perovskites, in polycrystalline thin
films but also perovskite nanoparticles (NPs) has
demonstrated excellent performance to implement a new
generation of photovoltaic and photonic devices. The
structural characterization of APbX3 thin films using
(scanning) transmission electron microscopy ((S)TEM)
techniques can provide valuable information that can be used
to understand and model their optoelectronic performance and
device properties. However, since APbX3 perovskites are soft
materials, their characterization using (S)TEM is
challenging. Here, we study and compare the structural
properties of two different metal halide APbX3 perovskite
thin films: bulk CH3NH3PbI3 prepared by spin-coating of the
precursors in solution and CsPbBr3 colloidal NPs synthetized
and deposited by doctor blading. Both specimen preparation
methods and working conditions for analysis by (S)TEM are
properly optimized. We show that CH3NH3PbI3 thin films grown
by a one-step method are composed of independent grains with
random orientations. The growth method results in the
formation of tetragonal perovskite thin films with good
adherence to an underlying TiO2 layer, which is
characterized by a photoluminescence (PL) emission band
centered at 775 nm. The perovskite thin films based on
CsPbBr3 colloidal NPs, which are used as the building blocks
of the film, are preserved by the deposition process, even
if small gaps are observed between adjacent NPs. The crystal
structure of CsPbBr3 NPs is cubic, which is beneficial for
optical properties due to its optimal band gap. The
absorption and PL spectra measured in both the thin film and
the colloidal solution of CsPbBr3 NPs are very similar,
indicating a good homogeneity of the thin films and the
absence of aggregation of NPs. However, a particular care
was required to avoid long electron irradiation times during
our structural studies, even at a low voltage of 80 kV, as
the material was observed to decompose through Pb
segregation.},
cin = {ER-C-1},
ddc = {530},
cid = {I:(DE-Juel1)ER-C-1-20170209},
pnm = {143 - Controlling Configuration-Based Phenomena (POF3-143)},
pid = {G:(DE-HGF)POF3-143},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:30620928},
UT = {WOS:000457725500001},
doi = {10.1088/1361-6528/aafc85},
url = {https://juser.fz-juelich.de/record/878293},
}